A Cryostat with a Window into Vacuum Ultraviolet ✛

Original: "An optical cryostat for automated testing of silicon photomultipliers with vacuum-ultraviolet light"
arXiv:2609.05840v1 · 2026-09-05 · CC BY 4.0 · 3 min
A setup that cools silicon photomultipliers down to 120 K and illuminates them with liquid xenon light to test their suitability for dark matter detectors.

The stage is bathed in icy light, and on it stand silicon spectators. Each is an array of tiny avalanche diodes capable of spotting a single photon, but only if the surrounding temperature drops to 165 K. Previously, such spectators were prepared for their performance one by one, by hand, and no one could guarantee they would perform uniformly on a large stage. Now, a temperature-controlled stage has been built for them, with a window transparent to ultraviolet light and a movable spotlight that can aim with precision to a tenth of a millimeter.

A silicon photomultiplier is an array of tiny avalanche diodes that count single photons. Vacuum ultraviolet is light with a wavelength shorter than 200 nm.

The spotlight here is not ordinary: it generates light from liquid xenon, the same light that flashes inside dark matter detectors. But ultraviolet at 175 nm is finicky, eagerly absorbed by moisture in the air. Therefore, the calcium fluoride window is constantly blown with dry nitrogen, much like wiping glasses before an important conversation. Behind the scenes, in a dark box, a cold is maintained with shiver-inducing stability: the temperature fluctuates by only 1.2 mK over ten minutes.

Ten spectators from the Hamamatsu array took the stage, and three things were measured for each. First, the dark count, meaning how many times the detector fires in complete darkness when no photons are present. Second, the charge of a single photoelectron, a tiny pulse of current born from a single photon. Third, the photon detection efficiency, the probability that a photon will actually produce a signal. At 165 K, it was 16.3%, and the temperature coefficient of breakdown voltage was (52.8±0.5) mV/K. This means that for each degree of warming, the detector needs a higher voltage to stay in shape.

Dark count is spurious firings without light. Photon detection efficiency is the probability that a photon will produce a signal. Overvoltage is the voltage above breakdown.

Previously, before this stage, no one could simultaneously cool a hundred such spectators and direct a beam of ultraviolet at each with millimeter precision. Commercial characterization systems are designed for room temperature, and single laboratory measurements do not provide statistics. Now there is a conveyor belt: load the array, set the coordinates, and the stage itself will put the spectator through all the tests. This fills the gap between a single experiment and industrial quality control.

The stage is already working for the nEXO collaboration, which is preparing a detector to search for neutrinoless double beta decay. There, thousands of silicon spectators with known characteristics are needed, and each must endure years in liquid xenon. Looking ahead, the same stage can be used to test how ultraviolet gradually degrades detectors and to build a model of spurious signals that hinder the discrimination of rare events. The icy light continues to fall on the silicon, and now it has an audience ready for the big premiere.

The calcium fluoride window transmits 88% of light at 172 nm, but it is so hygroscopic that it must be constantly flushed with dry nitrogen, otherwise moisture from the air absorbs the ultraviolet light.

Scientists
John BardeenLeo Esaki
Concepts
cryostat silicon photomultiplier thermal camera liquid helium temperature cryogenic sensing liquid helium photomultiplier tube cryogenic temperature rubidium vapor millikelvin lithium niobate